Up: Optimised polarimeter configurations for
In this appendix, we show that conditions 8 diagonalise
the error matrix
of the Stokes parameters and minimise
its determinant, if the noises in the n polarimeters have identical
levels and are not correlated.
We use the notation:
It can be seen from Eq. 7 that requiring that the
error on I be decorrelated from the errors on Q and U is
equivalent to the condition:
This condition can easily be fulfilled in a configuration where the
angles
are regularly distributed:
|  |
(A2) |
| |
In such configurations, Eq. (A1) becomes:
|  |
(A3) |
The solutions of Eq. (A3) under conditions (A2)
reduce to:
|  |
(A4) |
It is easily seen that conditions (A4) also automatically
ensure that S4 = 0
and therefore that
becomes diagonal and assumes the very
simple form:
|  |
(A5) |
independent of the orientation of the focal plane. Equation 9
is the consequence of A5.
The error volume is proportional to the determinant of the error
matrix
. Therefore, it is minimum when the
determinant of
(Eq. 7) is
maximum. This determinant can be written as:
| ![\begin{displaymath}
\mathrm{Det}(\bf{X}) =\\ \frac{1}{64}
\left[n^3 - n\,\vert ...
...^2(n - \vert S_4\vert\, \cos(\theta_4 - 2\,
\theta_2))\right].\end{displaymath}](/articles/aas/full/1999/06/ds7941/img86.gif) |
(A6) |
Because the Sk's are sums of n complex numbers with modulus 1, |Sk|
< n, and it is clear from Eq. A6 that
and that the upper bound is reached if and only if
Conditions (A2) and A4 have been shown above to
imply A7, and therefore ensure that
the determinant of the covariance matrix
is minimum.
Up: Optimised polarimeter configurations for
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